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		<id>http://wiki.panotools.org/index.php?title=Diffraction&amp;feed=atom&amp;action=history</id>
		<title>Diffraction - Revision history</title>
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		<updated>2013-05-24T09:46:30Z</updated>
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	<entry>
		<id>http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12958&amp;oldid=prev</id>
		<title>Erik Krause: zenitar and nikkor fisheye comparison regarding diffraction</title>
		<link rel="alternate" type="text/html" href="http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12958&amp;oldid=prev"/>
				<updated>2011-01-03T22:39:14Z</updated>
		
		<summary type="html">&lt;p&gt;zenitar and nikkor fisheye comparison regarding diffraction&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
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				&lt;col class='diff-content' /&gt;
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			&lt;tr valign='top'&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;← Older revision&lt;/td&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;Revision as of 22:39, 3 January 2011&lt;/td&gt;
			&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 32:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 32:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;===Wide angle===&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;===Wide angle===&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Although the above formula is applicable to wide angle and [[fisheye]] lenses as well it is harder to give correct values. Most DSLR wide angle and fisheye lenses change the entrance pupil diameter depending from the angle of incidence. This is intended and serves as a mechanism to compensate for natural [[vignetting]].&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Although the above formula is applicable to wide angle and [[fisheye]] lenses as well it is harder to give correct values. Most DSLR wide angle and fisheye lenses change the entrance pupil diameter depending from the angle of incidence. This is intended and serves as a mechanism to compensate for natural [[vignetting]].&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;However, diffraction is an issue for those lenses, too. For a comparison of two widely used fisheyes see [[Diffraction#External_links|link at the bottom]].&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Caveats==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Caveats==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 42:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 44:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*wikipedia on [[w:Angular resolution|Angular resolution]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*wikipedia on [[w:Angular resolution|Angular resolution]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*[http://www.kenrockwell.com/tech/focus.htm Ken Rockwell's page] on Selecting the Sharpest Aperture&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*[http://www.kenrockwell.com/tech/focus.htm Ken Rockwell's page] on Selecting the Sharpest Aperture&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;*[http://www.kenrockwell.com/zenit/zenitar-16mm.htm#sharp Ken Rockwell's page] with a sharpness comparison of the Zenitar 16mm and Nikkor 10.5mm fisheye lenses at different aperture.&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*A very extensive article about resolution limits on [http://www.luminous-landscape.com/tutorials/resolution.shtml Luminous Landscape] containing many valuable links.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*A very extensive article about resolution limits on [http://www.luminous-landscape.com/tutorials/resolution.shtml Luminous Landscape] containing many valuable links.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Erik Krause</name></author>	</entry>

	<entry>
		<id>http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12957&amp;oldid=prev</id>
		<title>Erik Krause: /* Resolution */  wide angle</title>
		<link rel="alternate" type="text/html" href="http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12957&amp;oldid=prev"/>
				<updated>2011-01-03T22:21:21Z</updated>
		
		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Resolution: &lt;/span&gt;  wide angle&lt;/span&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
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				&lt;col class='diff-content' /&gt;
			&lt;tr valign='top'&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;← Older revision&lt;/td&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;Revision as of 22:21, 3 January 2011&lt;/td&gt;
			&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 17:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 17:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160; &amp;lt;math&amp;gt; pixel resolution = \frac{FoV}{asin\left(\frac{1}{1490*D}\right)}&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160; &amp;lt;math&amp;gt; pixel resolution = \frac{FoV}{asin\left(\frac{1}{1490*D}\right)}&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;aperture&lt;/del&gt;, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in '''pixels/degree''' which is obtainable by a given focal length (vertical) and f-number (horizontal) without regard to currently available sensors for an ideal lens without aberrations:&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;physical &lt;/ins&gt;diameter of the lens' &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;[[entrance pupil]]&lt;/ins&gt;, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in '''pixels/degree''' which is obtainable by a given focal length (vertical) and f-number (horizontal) without regard to currently available sensors for an ideal lens without aberrations:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160;  '''50'''&amp;#160; &amp;#160; &amp;#160; 464&amp;#160; &amp;#160; 325&amp;#160; &amp;#160;  232&amp;#160; &amp;#160;  163&amp;#160; &amp;#160;  118&amp;#160; &amp;#160; &amp;#160; 81&amp;#160; &amp;#160; &amp;#160; 59&amp;#160; &amp;#160; 41&amp;#160; &amp;#160; 30&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160;  '''50'''&amp;#160; &amp;#160; &amp;#160; 464&amp;#160; &amp;#160; 325&amp;#160; &amp;#160;  232&amp;#160; &amp;#160;  163&amp;#160; &amp;#160;  118&amp;#160; &amp;#160; &amp;#160; 81&amp;#160; &amp;#160; &amp;#160; 59&amp;#160; &amp;#160; 41&amp;#160; &amp;#160; 30&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 29:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 29:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*You want to shoot a gigapixel panorama of 175° width with a 800mm lens at f/11. You get 175*1,891 = 330,925 pixel maximum horizontal resolution.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*You want to shoot a gigapixel panorama of 175° width with a 800mm lens at f/11. You get 175*1,891 = 330,925 pixel maximum horizontal resolution.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*You will use an APS-C format sensor in portrait orientation for this panorama. A 800mm lens has a FoV of 1.1° in that case, which at f/11 gives 2080 pixels or app. 6 megapixels. Applying the 70% rule to compensate for bayer interpolation blur indicates that 12 megapixels per image are enough.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*You will use an APS-C format sensor in portrait orientation for this panorama. A 800mm lens has a FoV of 1.1° in that case, which at f/11 gives 2080 pixels or app. 6 megapixels. Applying the 70% rule to compensate for bayer interpolation blur indicates that 12 megapixels per image are enough.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;===Wide angle===&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;Although the above formula is applicable to wide angle and [[fisheye]] lenses as well it is harder to give correct values. Most DSLR wide angle and fisheye lenses change the entrance pupil diameter depending from the angle of incidence. This is intended and serves as a mechanism to compensate for natural [[vignetting]].&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Caveats==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Caveats==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Erik Krause</name></author>	</entry>

	<entry>
		<id>http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12948&amp;oldid=prev</id>
		<title>Erik Krause: additional info</title>
		<link rel="alternate" type="text/html" href="http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12948&amp;oldid=prev"/>
				<updated>2010-12-29T12:43:08Z</updated>
		
		<summary type="html">&lt;p&gt;additional info&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
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				&lt;col class='diff-content' /&gt;
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				&lt;col class='diff-content' /&gt;
			&lt;tr valign='top'&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;← Older revision&lt;/td&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;Revision as of 12:43, 29 December 2010&lt;/td&gt;
			&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 5:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 5:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Sharpness==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Sharpness==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Diffraction is one of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;three &lt;/del&gt;factors limiting the image sharpness. Second is aberration (f.e. [[chromatic aberration]]) which is determined by lens build quality. Third is de-focus or [[Depth of Field]]. &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Diffraction is one of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;four lens based &lt;/ins&gt;factors limiting the image sharpness. Second is aberration (f.e. [[chromatic aberration]]) which is determined by lens build quality. Third is de-focus or [[Depth of Field]]&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. Fourth is motion blur due to lens shake&lt;/ins&gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Diffraction depends only on the physical aperture size. Hence it's effect is generally larger the smaller the used sensor is due to the larger magnification of the image. That's the reason why compact cameras can't (or shouldn't) be stopped down further than f/5.6. As a rule of thumb the limit for APS-C sized sensors is f/8 to f/11 and for full frame ones f/16 to f/22.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Diffraction depends only on the physical aperture size. Hence it's effect is generally larger the smaller the used sensor is due to the larger magnification of the image. That's the reason why compact cameras can't (or shouldn't) be stopped down further than f/5.6. As a rule of thumb the limit for APS-C sized sensors is f/8 to f/11 and for full frame ones f/16 to f/22.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 12:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 12:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Resolution==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Resolution==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm. The resulting formula is:&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. We can safely assume the equivalent of one pixel distance as the minimum resolvable distance required by the Rayleigh criterion&lt;/ins&gt;. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;&amp;lt;math&amp;gt; pixel resolution = \frac{FoV}{asin\left(\frac{1}{1490*D}\right)}&amp;lt;/math&amp;gt;&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in '''pixels/degree''' which is obtainable by a given focal length (vertical) and f-number (horizontal) without regard to currently available sensors:&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm which is in the middle of the spectrum and a color where our eyes are most sensitive. The resulting formula is:&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt; &amp;lt;math&amp;gt; pixel resolution = \frac{FoV}{asin\left(\frac{1}{1490*D}\right)}&amp;lt;/math&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in '''pixels/degree''' which is obtainable by a given focal length (vertical) and f-number (horizontal) without regard to currently available sensors &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;for an ideal lens without aberrations&lt;/ins&gt;:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160;  '''50'''&amp;#160; &amp;#160; &amp;#160; 464&amp;#160; &amp;#160; 325&amp;#160; &amp;#160;  232&amp;#160; &amp;#160;  163&amp;#160; &amp;#160;  118&amp;#160; &amp;#160; &amp;#160; 81&amp;#160; &amp;#160; &amp;#160; 59&amp;#160; &amp;#160; 41&amp;#160; &amp;#160; 30&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160;  '''50'''&amp;#160; &amp;#160; &amp;#160; 464&amp;#160; &amp;#160; 325&amp;#160; &amp;#160;  232&amp;#160; &amp;#160;  163&amp;#160; &amp;#160;  118&amp;#160; &amp;#160; &amp;#160; 81&amp;#160; &amp;#160; &amp;#160; 59&amp;#160; &amp;#160; 41&amp;#160; &amp;#160; 30&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 23:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 25:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; '''800'''&amp;#160; &amp;#160; 7,430&amp;#160; 5,201&amp;#160;  3,715&amp;#160;  2,601&amp;#160;  1,891&amp;#160;  1,300&amp;#160; &amp;#160;  946&amp;#160;  650&amp;#160;  473&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; '''800'''&amp;#160; &amp;#160; 7,430&amp;#160; 5,201&amp;#160;  3,715&amp;#160;  2,601&amp;#160;  1,891&amp;#160;  1,300&amp;#160; &amp;#160;  946&amp;#160;  650&amp;#160;  473&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160; '''1200'''&amp;#160;  11,145&amp;#160; 7,802&amp;#160;  5,573&amp;#160;  3,901&amp;#160;  2,837&amp;#160;  1,950&amp;#160;  1,418&amp;#160;  975&amp;#160;  709&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160; '''1200'''&amp;#160;  11,145&amp;#160; 7,802&amp;#160;  5,573&amp;#160;  3,901&amp;#160;  2,837&amp;#160;  1,950&amp;#160;  1,418&amp;#160;  975&amp;#160;  709&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Some usage examples&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Some usage examples&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*You want to shoot a gigapixel panorama of 175° width with a 800mm lens at f/11. You get 175*1,891 = 330,925 pixel maximum horizontal resolution.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*You want to shoot a gigapixel panorama of 175° width with a 800mm lens at f/11. You get 175*1,891 = 330,925 pixel maximum horizontal resolution.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*You will use an APS-C format sensor in portrait orientation for this panorama. A 800mm lens has a FoV of 1.1° in that case, which at f/11 gives 2080 pixels or app. 6 megapixels. Applying the 70% rule to compensate for bayer interpolation blur indicates that 12 megapixels per image are enough.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*You will use an APS-C format sensor in portrait orientation for this panorama. A 800mm lens has a FoV of 1.1° in that case, which at f/11 gives 2080 pixels or app. 6 megapixels. Applying the 70% rule to compensate for bayer interpolation blur indicates that 12 megapixels per image are enough.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;==Caveats==&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;Unfortunately most lenses are diffraction limited at small apertures only. Since most lens aberrations get better the further you stop down, it might be that shooting wide open gives you worse results than fully stopped down. Hence the real sharpest aperture of a particular lens must be determined by experiment.&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;Other factors (lens shake, atmospheric scintillation, sensor noise, haze etc.) reduce resolution and sharpness even further, hence the above values will seldom be reached.&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==External links==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==External links==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 31:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 39:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*wikipedia on [[w:Angular resolution|Angular resolution]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*wikipedia on [[w:Angular resolution|Angular resolution]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*[http://www.kenrockwell.com/tech/focus.htm Ken Rockwell's page] on Selecting the Sharpest Aperture&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;*[http://www.kenrockwell.com/tech/focus.htm Ken Rockwell's page] on Selecting the Sharpest Aperture&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;color: red; font-weight: bold; text-decoration: none;&quot;&gt;*A very extensive article about resolution limits on [http://www.luminous-landscape.com/tutorials/resolution.shtml Luminous Landscape] containing many valuable links.&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Erik Krause</name></author>	</entry>

	<entry>
		<id>http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12940&amp;oldid=prev</id>
		<title>Thomas Rauscher: Fixed math bug. Original formular by Erik</title>
		<link rel="alternate" type="text/html" href="http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12940&amp;oldid=prev"/>
				<updated>2010-12-27T14:44:34Z</updated>
		
		<summary type="html">&lt;p&gt;Fixed math bug. Original formular by Erik&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
			&lt;tr valign='top'&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;← Older revision&lt;/td&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;Revision as of 14:44, 27 December 2010&lt;/td&gt;
			&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 13:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 13:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Resolution==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Resolution==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution. For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm. The resulting formula is:&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution. For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm. The resulting formula is:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt; [[File:pixelresolution.png]] &lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;lt;math&amp;gt; pixel resolution = \frac{FoV}{asin\left(\frac{1}{1490*D}\right)}&amp;lt;/math&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in '''pixels/degree''' which is obtainable by a given focal length (vertical) and f-number (horizontal) without regard to currently available sensors:&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in '''pixels/degree''' which is obtainable by a given focal length (vertical) and f-number (horizontal) without regard to currently available sensors:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Thomas Rauscher</name></author>	</entry>

	<entry>
		<id>http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12934&amp;oldid=prev</id>
		<title>Erik Krause: /* Resolution */ clarified</title>
		<link rel="alternate" type="text/html" href="http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12934&amp;oldid=prev"/>
				<updated>2010-12-25T22:09:13Z</updated>
		
		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Resolution: &lt;/span&gt; clarified&lt;/span&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
			&lt;tr valign='top'&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;← Older revision&lt;/td&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;Revision as of 22:09, 25 December 2010&lt;/td&gt;
			&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 14:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 14:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution. For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm. The resulting formula is:&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution. For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm. The resulting formula is:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160; [[File:pixelresolution.png]] &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160; [[File:pixelresolution.png]] &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in pixels/degree which is obtainable by a given focal length (vertical) and f-number (horizontal):&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;'''&lt;/ins&gt;pixels/degree&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;''' &lt;/ins&gt;which is obtainable by a given focal length (vertical) and f-number (horizontal) &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;without regard to currently available sensors&lt;/ins&gt;:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160;  '''50'''&amp;#160; &amp;#160; &amp;#160; 464&amp;#160; &amp;#160; 325&amp;#160; &amp;#160;  232&amp;#160; &amp;#160;  163&amp;#160; &amp;#160;  118&amp;#160; &amp;#160; &amp;#160; 81&amp;#160; &amp;#160; &amp;#160; 59&amp;#160; &amp;#160; 41&amp;#160; &amp;#160; 30&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160;  '''50'''&amp;#160; &amp;#160; &amp;#160; 464&amp;#160; &amp;#160; 325&amp;#160; &amp;#160;  232&amp;#160; &amp;#160;  163&amp;#160; &amp;#160;  118&amp;#160; &amp;#160; &amp;#160; 81&amp;#160; &amp;#160; &amp;#160; 59&amp;#160; &amp;#160; 41&amp;#160; &amp;#160; 30&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Erik Krause</name></author>	</entry>

	<entry>
		<id>http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12933&amp;oldid=prev</id>
		<title>Erik Krause: /* Resolution */</title>
		<link rel="alternate" type="text/html" href="http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12933&amp;oldid=prev"/>
				<updated>2010-12-25T21:33:28Z</updated>
		
		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Resolution&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
			&lt;tr valign='top'&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;← Older revision&lt;/td&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;Revision as of 21:33, 25 December 2010&lt;/td&gt;
			&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 13:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 13:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Resolution==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Resolution==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution. For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm. The resulting formula is:&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution. For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm. The resulting formula is:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160; &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;&amp;lt;math&amp;gt; pixel resolution = \frac{FoV}{asin\left(\frac{1}{1490*D}\right)}\,\!&amp;lt;/math&amp;gt; &lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160; &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;[[File:pixelresolution.png]] &lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in pixels/degree which is obtainable by a given focal length (vertical) and f-number (horizontal):&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in pixels/degree which is obtainable by a given focal length (vertical) and f-number (horizontal):&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Erik Krause</name></author>	</entry>

	<entry>
		<id>http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12931&amp;oldid=prev</id>
		<title>Erik Krause: /* Sharpness */</title>
		<link rel="alternate" type="text/html" href="http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12931&amp;oldid=prev"/>
				<updated>2010-12-25T20:46:39Z</updated>
		
		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Sharpness&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
			&lt;tr valign='top'&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;← Older revision&lt;/td&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;Revision as of 20:46, 25 December 2010&lt;/td&gt;
			&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 7:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 7:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Diffraction is one of three factors limiting the image sharpness. Second is aberration (f.e. [[chromatic aberration]]) which is determined by lens build quality. Third is de-focus or [[Depth of Field]]. &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Diffraction is one of three factors limiting the image sharpness. Second is aberration (f.e. [[chromatic aberration]]) which is determined by lens build quality. Third is de-focus or [[Depth of Field]]. &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Diffraction depends only on the physical aperture size. Hence it's effect is generally larger the smaller the used sensor is due to the larger magnification of the image. That's the reason why compact cameras can't (or shouldn't) be stopped down further than f/5.6. As a rule of thumb the limit for APS-C sized sensors is f/8 to f/11 and for full frame ones f/16 to f/22. &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;Diffraction depends only on the physical aperture size. Hence it's effect is generally larger the smaller the used sensor is due to the larger magnification of the image. That's the reason why compact cameras can't (or shouldn't) be stopped down further than f/5.6. As a rule of thumb the limit for APS-C sized sensors is f/8 to f/11 and for full frame ones f/16 to f/22&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;.&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;You can balance [[Depth of Field]] against diffraction. An approach is the sharpest aperture. [[Diffraction#External_links|See link at the bottom]]&lt;/ins&gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Resolution==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Resolution==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Erik Krause</name></author>	</entry>

	<entry>
		<id>http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12930&amp;oldid=prev</id>
		<title>Erik Krause: /* Resolution */ tried to fix math...</title>
		<link rel="alternate" type="text/html" href="http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12930&amp;oldid=prev"/>
				<updated>2010-12-25T20:34:45Z</updated>
		
		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Resolution: &lt;/span&gt; tried to fix math...&lt;/span&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
			&lt;tr valign='top'&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;← Older revision&lt;/td&gt;
			&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;Revision as of 20:34, 25 December 2010&lt;/td&gt;
			&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 11:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 11:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Resolution==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;==Resolution==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution. For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm. The resulting formula is:&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution. For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm. The resulting formula is:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160; &amp;lt;math&amp;gt; pixel resolution = &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;/&lt;/del&gt;frac {FoV}{asin \left(\frac{1}{1490*D}\right)}&amp;lt;/math&amp;gt; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160; &amp;lt;math&amp;gt; pixel resolution = &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;\&lt;/ins&gt;frac{FoV}{asin\left(\frac{1}{1490*D}\right)}&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;\,\!&lt;/ins&gt;&amp;lt;/math&amp;gt; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in pixels/degree which is obtainable by a given focal length (vertical) and f-number (horizontal):&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in pixels/degree which is obtainable by a given focal length (vertical) and f-number (horizontal):&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&amp;#160; &amp;#160; &amp;#160; &amp;#160; &amp;#160;  '''2.8&amp;#160; &amp;#160; &amp;#160; 4&amp;#160; &amp;#160;  5.6&amp;#160; &amp;#160; &amp;#160;  8&amp;#160; &amp;#160; &amp;#160; 11&amp;#160; &amp;#160; &amp;#160; 16&amp;#160; &amp;#160; &amp;#160; 22&amp;#160; &amp;#160; 32&amp;#160; &amp;#160; 44'''&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Erik Krause</name></author>	</entry>

	<entry>
		<id>http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12929&amp;oldid=prev</id>
		<title>Erik Krause: basic page on diffraction regarding panoramas</title>
		<link rel="alternate" type="text/html" href="http://wiki.panotools.org/index.php?title=Diffraction&amp;diff=12929&amp;oldid=prev"/>
				<updated>2010-12-25T20:23:55Z</updated>
		
		<summary type="html">&lt;p&gt;basic page on diffraction regarding panoramas&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Glossary|The physical property of light which causes image blur depending from the aperture used.}}&lt;br /&gt;
&lt;br /&gt;
==What it is==&lt;br /&gt;
Diffraction in general is the bending of waves around an obstacle. In photography the light waves are bent around the edges of the aperture, causing f.e. the well known star like pattern around the sun if shot stopped down. Since diffraction affects any point of the image (not only very bright sources) it reduces general sharpness and limits effective resolution. Diffraction blurs any point to a pattern called &amp;quot;[[w:Airy disk]]&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
==Sharpness==&lt;br /&gt;
Diffraction is one of three factors limiting the image sharpness. Second is aberration (f.e. [[chromatic aberration]]) which is determined by lens build quality. Third is de-focus or [[Depth of Field]]. &lt;br /&gt;
&lt;br /&gt;
Diffraction depends only on the physical aperture size. Hence it's effect is generally larger the smaller the used sensor is due to the larger magnification of the image. That's the reason why compact cameras can't (or shouldn't) be stopped down further than f/5.6. As a rule of thumb the limit for APS-C sized sensors is f/8 to f/11 and for full frame ones f/16 to f/22. &lt;br /&gt;
&lt;br /&gt;
==Resolution==&lt;br /&gt;
The maximum obtainable resolution is limited by diffraction according to the [[w:angular resolution|Rayleigh criterion]]. Since this criterion defines the angular resolution it can be directly used for zoomable panoramas neglecting sensor sizes etc. By simply dividing the panorama [[Field of View]] (FoV) by the angular resolution we get the maximum possible pixel resolution. For an average value we take the wavelength of light ''λ'' = 550nm = 5.5*10&amp;lt;sup&amp;gt;-4&amp;lt;/sup&amp;gt;mm. The resulting formula is:&lt;br /&gt;
 &amp;lt;math&amp;gt; pixel resolution = /frac {FoV}{asin \left(\frac{1}{1490*D}\right)}&amp;lt;/math&amp;gt; &lt;br /&gt;
''D'' is the diameter of the lens' aperture, which is the focal length in mm divided by the f-number. The following table shows the maximum angular resolution in pixels/degree which is obtainable by a given focal length (vertical) and f-number (horizontal):&lt;br /&gt;
           '''2.8      4     5.6       8      11      16      22    32    44'''&lt;br /&gt;
   '''50'''      464    325     232     163     118      81      59    41    30&lt;br /&gt;
  '''100'''      929    650     464     325     236     163     118    81    59&lt;br /&gt;
  '''200'''    1,858  1,300     929     650     473     325     236   163   118&lt;br /&gt;
  '''400'''    3,715  2,601   1,858   1,300     946     650     473   325   236&lt;br /&gt;
  '''800'''    7,430  5,201   3,715   2,601   1,891   1,300     946   650   473&lt;br /&gt;
 '''1200'''   11,145  7,802   5,573   3,901   2,837   1,950   1,418   975   709&lt;br /&gt;
Some usage examples&lt;br /&gt;
*You want to shoot a gigapixel panorama of 175° width with a 800mm lens at f/11. You get 175*1,891 = 330,925 pixel maximum horizontal resolution.&lt;br /&gt;
*You will use an APS-C format sensor in portrait orientation for this panorama. A 800mm lens has a FoV of 1.1° in that case, which at f/11 gives 2080 pixels or app. 6 megapixels. Applying the 70% rule to compensate for bayer interpolation blur indicates that 12 megapixels per image are enough.&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
*wikipedia on [[w:Diffraction|Diffraction]]&lt;br /&gt;
*wikipedia on [[w:Angular resolution|Angular resolution]]&lt;br /&gt;
*[http://www.kenrockwell.com/tech/focus.htm Ken Rockwell's page] on Selecting the Sharpest Aperture&lt;/div&gt;</summary>
		<author><name>Erik Krause</name></author>	</entry>

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